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Complete tracking of transient proton flow through active chloroplast ATP synthase.

Proton pumping in thylakoid membranes and backflow of protons through the active ATP synthase CF0-CF1 (where CF0 is the proton channel and CF1 is the catalytic portion) were investigated by flash spectrophotometry. A steady pH difference across the membrane was generated by continuous measuring light, supplemented by voltage transients that were generated by flashing light. In the presence of P(i) and ADP, the electric potential transients elicited transients of proton flow via CF0-CF1, typically 1.3 H(+) per CF1 and flash group. Proton flow was blocked by CF0-CF1 inhibitors: N,N'-dicyclohexylcarbodiimide, acting on the channel component CF0, and tentoxin, acting on the catalytic component CF1. The half-rise time was 40 ms in (1)H(2)O and 78 ms in (2)H(2)O. ATP synthesis under conditions of flashing light and transient proton flow was characterized by a K(m)(P(i)) of only 14 muM, contrasting with a K(m) of several hundred micromolar for continuous ATP synthesis at high rate. This might reflect a resistance to P(i) diffusion. The degree of proton delocalization in the chemiosmotic coupling between redox reactions and ATP synthesis is under debate. In thylakoids, it has been proposed that intramembrane proton buffering domains act as ducts for protons between pumps and ATP synthases. In this work, transient proton flow by way of CF0-CF1 was completely tracked from the lumen, across the membrane, and into the suspending medium. Proton uptake from the lumen and charge flow across the membrane occurred synchronously and in stoichiometric proportion. The uptake of protons from the lumen by CF0-CF1, half completed in 40 ms, was preceded by release of protons from water oxidation into the lumen, half completed in <1 ms. Hence, pumps and ATP synthases were coupled through the lumen without involvement of intramembrane domains.

Journal Article↗

Conformation of the glycotripeptide repeating unit of antifreeze glycoprotein of polar fish as determined from the fully assigned proton n.m.r. spectrum.

With its simple glycotripeptide repeating structure the antifreeze glycoprotein of polar fish may be an especially simple conformational mode for mucin glycoproteins with similar but more complex structures. The fully assigned proton n.m.r. spectrum confirms the anomeric configurations of the hexapyranosidic sugars of the side chains and the coupling constants of the alpha GalNAc and the beta Gal residues show both to be in the expected 4C1 chair conformation. The assignment of a single resonance for each proton of the (Ala-Thr-Ala)n repeat unit coupled with the observation of long range nuclear Overhauser effects (n.O.e.) implies a three-fold repeating conformation. The resonances of the two alanines are distinct and can be assigned to their correct positions in the peptide sequence by n.O.e. observed at the amide proton resonances on saturation of the alpha proton signals. The amide proton coupling constants of all three peptide residues are similar and imply a limited range of peptide backbone torsion angles, phi CN. The large n.O.e. which has been observed between the amide proton and the alpha proton of the residue preceding it in the sequence implies large positive values for the peptide dihedral angle, psi CC. Limits are placed on possible values of side chain dihedral angles by the observation of the coupling constant between the alpha and beta protons of the threonyl residue. The observation of n.O.e. between the anomeric proton of GalNAc and the threonyl side chain protons gives information on the conformation of the alpha glycosidic linkage between the disaccharide and the peptide. n.O.e. observed between the protons of the beta glycosidic linkage indicates the conformation of the disaccharide and the large amide proton coupling constant of the GalNAc residue shows a trans proton relationship. The spectroscopically derived data have been combined with conformational energy calculations to give a conformational model for antifreeze glycoprotein in which the hydrophobic surfaces of the disaccharide side chains are wrapped closely against a three-fold left handed helical peptide backbone. The hydrophilic sides of the disaccharides are aligned so that they may bind to the ice crystal face, which is perpendicular to the fast growth axis inhibiting normal crystal growth.

Animals↗

A treatment planning comparison of intensity modulated photon and proton therapy for paraspinal sarcomas.

PURPOSE: A comparative treatment planning study has been undertaken between intensity modulated (IM) photon therapy and IM proton therapy (IMPT) in paraspinal sarcomas, so as to assess the potential benefits and limitations of these treatment modalities. In the case of IM proton therapy, plans were compared also for two different sizes of the pencil beam. Finally, a 10% and 20% dose escalation with IM protons was planned, and the consequential organ at risk (OAR) irradiation was evaluated. METHODS AND MATERIALS: Plans for 5 patients were computed for IM photons (7 coplanar fields) and protons (3 coplanar beams), using the KonRad inverse treatment planning system (developed at the German Cancer Research Center). IMPT planning was performed assuming 2 different sizes of the pencil beam: IMPT with a beam of full width at half-maximum of 20 mm, and IMPT with a "mini-beam" (IMPT(M), full width at half-maximum = 12 mm). Prescribed dose was 77.4 Gy or cobalt Gray equivalent (CGE) for protons to the gross tumor volume (GTV). Surface and center spinal cord dose constraint for all techniques was 64 and 53 Gy/CGE, respectively. Tumor and OAR dose-volume histograms were calculated. Results were analyzed using dose-volume histogram parameters, inhomogeneity coefficient, and conformity index. RESULTS: Gross tumor volume coverage was optimal and equally homogeneous with both IM photon and IM proton plans. Compared to the IM photon plans, the use of IM proton beam therapy leads to a substantial reduction of the OAR total integral dose in the low-level to mid-dose level. Median heart, lung, kidney, stomach, and liver mean dose and dose at the 50% volume level were consistently reduced by a factor of 1.3 to 25. Tumor dose homogeneity in IMPT(M) plans was always better than with IMPT planning (median inhomogeneity coefficient, 0.19 vs. 0.25). IMPT dose escalation (to 92.9 CGE to the GTV) was possible in all patients without exceeding the normal-tissue dose limits. CONCLUSIONS: These results suggest that the use of IM photon therapy, when compared to IM protons, can result in similar levels of tumor conformation. IM proton therapy, however, reduces the OAR integral dose substantially, compared to IM photon radiation therapy. As a result, tumor dose escalation was always possible with IM proton planning, within the maximal OAR dose constraints. In IM proton planning, reducing the size of the proton pencil beam (using the "mini-beam") improved the dose homogeneity, but it did not have a significant effect on the dose conformity.

Humans↗

Protons, the thylakoid membrane, and the chloroplast ATP synthase.

According to the chemiosmotic theory, proton pumps and ATP synthases are coupled by lateral proton flow through aqueous phases. Three long-standing challenges to this concept, all of which have been loosely subsumed under 'localized coupling' in the literature, were examined in the light of experiments carried out with thylakoids: (1) Nearest neighbor interaction between pumps and ATP synthases. Considering the large distances between photosystem II and CFoCF1, in stacked thylakoids this is a priori absent. (2) Enhanced proton diffusion along the surface of the membrane. This could not be substantiated for the outer side of the thylakoid membrane. Even for the interface between pure lipid and water, two laboratories have reported the absence of enhanced diffusion. (3) Localized proton ducts in the membrane. Intramembrane domains that can transiently trap protons do exist in thylakoid membranes, but because of their limited storage capacity for protons, they probably do not matter for photophosphorylation under continuous light. Seemingly in favor of localized proton ducts is the failure of a supposedly permeant buffer to enhance the onset lag of photophosphorylation. However, it was found that failure of some buffers and the ability of others in this respect were correlated with their failure/ability to quench pH transients in the thylakoid lumen, as predicted by the chemiosmotic theory. It was shown that the chemiosmotic concept is a fair approximation, even for narrow aqueous phases, as in stacked thylakoids. These are approximately isopotential, and protons are taken in by the ATP synthase straight from the lumen. The molecular mechanism by which F0F1 ATPases couple proton flow to ATP synthesis is still unknown. The threefold structural symmetry of the headpiece that, probably, finds a corollary in the channel portion of these enzymes appeals to the common wisdom that structural symmetry causes functional symmetry. "Rotation catalysis" has been proposed. It is of heuristic value to visualize CFoCF1 as a mechanical coupling device. Its maximum turnover number ranges up to 400 s-1 for ATP and 1200 s-1 for protons. At about 200 mV electric driving force this implied a conductance of about 1 fS. Its channel portion (CFo), however, has revealed a very large protonic conductance of 1 pS (three orders of magnitude greater than the protonic conductance of gramicidin around neutral pH). (6) The sight and smell of food increased LH serotonin release; this effect was detectable when local fluoxetine was used to block serotonin reuptake.(ABSTRACT TRUNCATED AT 400 WORDS)

Biological Transport↗

Proton permeation of lipid bilayers.

Proton permeation of the lipid bilayer barrier has two unique features. First, permeability coefficients measured at neutral pH ranges are six to seven orders of magnitude greater than expected from knowledge of other monovalent cations. Second, proton conductance across planar lipid bilayers varies at most by a factor of 10 when pH is varied from near 1 to near 11. Two mechanisms have been proposed to account for this anomalous behavior: proton conductance related to contaminants of lipid bilayers, and proton translocation along transient hydrogen-bonded chains (tHBC) of associated water molecules in the membrane. The weight of evidence suggests that trace contaminants may contribute to proton conductance across planar lipid membranes at certain pH ranges, but cannot account for the anomalous proton flux in liposome systems. Two new results will be reported here which were designed to test the tHBC model. These include measurements of relative proton/potassium permeability in the gramicidin channel, and plots of proton flux against the magnitude of pH gradients. (1) The relative permeabilities of protons and potassium through the gramicidin channel, which contains a single strand of hydrogen-bonded water molecules, were found to differ by at least four orders of magnitude when measured at neutral pH ranges. This result demonstrates that a hydrogen-bonded chain of water molecules can provide substantial discrimination between protons and other cations. It was also possible to calculate that if approximately 7% of bilayer water was present in a transient configuration similar to that of the gramicidin channel, it could account for the measured proton flux. (2) The plot of proton conductance against pH gradient across liposome membranes was superlinear, a result that is consistent with one of three alternative tHBC models for proton conductance described by Nagle elsewhere in this volume.

Biological Transport↗

Electron and proton transport across the plasma membrane.

Transplasm membrane electron transport in both plant and animal cells activates proton release. The nature and components of the electron transport system and the mechanism by which proton release is activated remains to be discovered. Reduced pyridine nucleotides are substrates for the plasma membrane dehydrogenases. Both plant and animal membranes have unusual cyanide-insensitive oxidases so oxygen can be the natural electron acceptor. Natural ferric chelates or ferric transferrin can also act as electron acceptors. Artificial, impermeable oxidants such as ferricyanide are used to probe the activity. Since plasma membranes contain b cytochromes, flavin, iron, and quinones, components for electron transport are present but their participation, except for quinone, has not been demonstrated. Stimulation of electron transport with impermeable oxidants and hormones activates proton release from cells. In plants the electron transport and proton release is stimulated by red or blue light. Inhibitors of electron transport, such as certain antitumor drugs, inhibit proton release. With animal cells the high ratio of protons released to electrons transferred, stimulation of proton release by sodium ions, and inhibition by amilorides indicates that electron transport activates the Na+/H+ antiport. In plants part of the proton release can be achieved by activation of the H+ ATPase. A contribution to proton transfer by protonated electron carriers in the membrane has not been eliminated. In some cells transmembrane electron transport has been shown to cause cytoplasmic pH changes or to stimulate protein kinases which may be the basis for activation of proton channels in the membrane. The redox-induced proton release causes internal and external pH changes which can be related to stimulation of animal and plant cell growth by external, impermeable oxidants or by oxygen.

Adenosine Triphosphatases↗

A method for writing enzyme rate equations: application to the estimation of the number and size of key proton families.

We develop a method to derive the rate equation for enzyme models that include pH-dependent activation. Our presentation is based on a kinetic model recently described for sucrase, the three-key-proton model of Vasseur and coworkers, which considers the existence, in the acid ionization reaction, of two functionally distinct prototropic groups, respectively responsible for either V-type or K-type kinetic effects. In contrast, as concerns the basic ionization reaction, the model conforms to classical concepts of pH-dependent activation, whereby a single proton participates in either V-type or K-type effects but not in both at the same time. Enzymes with more than three key protons have been described, indicating that, rather than isolated protons, groups of protons should be considered, and therefore the model can be better described as a three-proton-family model, where a proton family is defined as one or several protons that are gained or lost as a block and perform the same kinetic function. The resulting model is treated here as a useful framework upon which other models can be built. To facilitate the writing of the rate equations, we define two new entities: (1) intralevel coefficients, which describe the various combinations of the enzyme with either the substrate(s), the allosteric effector(s), or both at a given protonation level, and (2) interlevel coefficients, which describe the interplay between the various protonation levels. The resulting rate equation can be used in a global fit procedure permitting in a single computer run the estimation of (1) the entire set of dissociation and microscopic ionization constants of the model, (2) the number and kinetic function of proton families characterizing the enzyme under consideration, and (3) the number of key protons constituting each family, which is derived from the derivatives of the kinetic parameters, Vm/Km, Vm, and Km.

Enzymes↗

Sensitivity and resolution in proton solid-state NMR at intermediate deuteration levels: quantitative linewidth characterization and applications to correlation spectroscopy.

We present a systematic study of proton linewidths in rigid solids as a function of sample spinning frequency and proton density, with the latter controlled by the ratio of protonated and perdeuterated model compounds. We find that the linewidth correlates more closely with the overall proton density (rho(H)) than the size of local clusters of (1)H spins. At relatively high magic-angle spinning (MAS) rates, the linewidth depends linearly upon the inverse MAS rate. In the limit of infinite spinning rate and/or zero proton concentration, the linewidth extrapolates to a non-zero value, owing to contributions from scalar couplings, chemical shift dispersion, and B(0) field inhomogeneity. The slope of this line depends on the overall concentration of unexchangeable protons in the sample and the spinning rate. At up to 30% protonation levels ( approximately 2 (1)H/100A(3)), proton detection experiments are demonstrated to have a substantial (2- to 3-fold) sensitivity gain over corresponding (13)C-detected experiments. Within this range, the absolute sensitivity increases with protonation level; the optimal compromise between sensitivity and resolution is in the range of 20-30% protonation. We illustrate the use of dilute protons for polarization transfer to and from low-gamma spins within 5A, and to be utilized as both magnetization source and detection spins. The intermediate protonation regime enhances relaxation properties, which we expect will enable new types of (1)H correlation pulse sequences to be implemented with improved resolution and sensitivity.

Alanine↗

Protonation reactions and their coupling in bacteriorhodopsin.

Light-induced changes of the proton affinities of amino acid side groups are the driving force for proton translocation in bacteriorhodopsin. Recent progress in obtaining structures of bacteriorhodopsin and its intermediates with an increasingly higher resolution, together with functional studies utilizing mutant pigments and spectroscopic methods, have provided important information on the molecular architecture of the proton transfer pathways and the key groups involved in proton transport. In the present paper I consider mechanisms of light-induced proton release and uptake and intramolecular proton transport and mechanisms of modulation of proton affinities of key groups in the framework of these data. Special attention is given to some important aspects that have surfaced recently. These are the coupling of protonation states of groups involved in proton transport, the complex titration of the counterion to the Schiff base and its origin, the role of the transient protonation of buried groups in catalysis of the chromophore's thermal isomerization, and the relationship between proton affinities of the groups and the pH dependencies of the rate constants of the photocycle and proton transfer reactions.

Amino Acids↗

Electron-proton interactions in terminal oxidases.

The cytochrome c and ubiquinol oxidases discussed in this article are membrane-bound redox-driven proton pumps which couple an electron current to a proton current across the membrane. This coupling requires a control of the thermodynamics and/or rates of internal electron- and proton-transfer reactions (termed 'gating'). Therefore, to understand the structure-function relation of these proton pumps, individual electron- and proton-transfer reactions must be investigated. We have undertaken such studies by using a combination of site-directed mutagenesis and spectroscopic techniques. The results show that proton uptake/release upon reduction/oxidation of heme a3 takes place on a ms-time scale through the K-pathway (including Thr(I-359) and Lys(I-362)), but not through the D-pathway (including Asp(I-132) and Glu(I-286)). During reaction of the reduced enzyme with O2, both substrate and pumped protons are taken up through the D-pathway (but not through the K-pathway) in a biphasic process with time constants of 100 microseconds and 1 ms. Thus, the original assignment of the role of the D-pathway (used only for pumped protons) must be revised. Dynamic studies of proton uptake to the enzyme surface show that on the proton-input side, the surface carries a proton-collecting antenna made of carboxylate and histidine residues which enable the enzyme to pick up protons with a rate compatible to the enzyme turnover rate. These results are consistent with the three-dimensional cytochrome c oxidase structure which shows that the entry point to the D-pathway (but not to the K-pathway) is surrounded by a network of histidine residues within a negative electrostatic potential.

Biological Transport↗

Structure and dynamics of a proton wire: a theoretical study of H+ translocation along the single-file water chain in the gramicidin A channel.

The rapid translocation of H+ along a chain of hydrogen-bonded water molecules, or proton wire, is thought to be an important mechanism for proton permeation through transmembrane channels. Computer simulations are used to study the properties of the proton wire formed by the single-file waters in the gramicidin A channel. The model includes the polypeptidic dimer, with 22 water molecules and one excess proton. The dissociation of the water molecules is taken into account by the "polarization model" of Stillinger and co-workers. The importance of quantum effects due to the light mass of the hydrogen nuclei is examined with the use of discretized Feynman path integral molecular dynamics simulations. Results show that the presence of an excess proton in the pore orients the single-file water molecules and affects the geometry of water-water hydrogen bonding interactions. Rather than a well-defined hydronium ion OH3+ in the single-file region, the protonated species is characterized by a strong hydrogen bond resembling that of O2H5+. The quantum dispersion of protons has a small but significant effect on the equilibrium structure of the hydrogen-bonded water chain. During classical trajectories, proton transfer between consecutive water molecules is a very fast spontaneous process that takes place in the subpicosecond time scale. The translocation along extended regions of the chain takes place neither via a totally concerted mechanism in which the donor-acceptor pattern would flip over the entire chain in a single step, nor via a succession of incoherent hops between well-defined intermediates. Rather, proton transfer in the wire is a semicollective process that results from the subtle interplay of rapid hydrogen-bond length fluctuations along the water chain. These rapid structural fluctuations of the protonated single file of waters around an average position and the slow movements of the average position of the excess proton along the channel axis occur on two very different time scales. Ultimately, it is the slow reorganization of hydrogen bonds between single-file water molecules and channel backbone carbonyl groups that, by affecting the connectivity and the dynamics of the single-file water chain, also limits the translocation of the proton across the pore.

Biophysical Phenomena↗

Coupling of drug protonation to the specific binding of aminoglycosides to the A site of 16 S rRNA: elucidation of the number of drug amino groups involved and their identities.

2-Deoxystreptamine (2-DOS) aminoglycoside antibiotics bind specifically to the central region of the 16S rRNA A site and interfere with protein synthesis. Recently, we have shown that the binding of 2-DOS aminoglycosides to an A site model RNA oligonucleotide is linked to the protonation of drug amino groups. Here, we extend these studies to define the number of amino groups involved as well as their identities. Specifically, we use pH-dependent 15N NMR spectroscopy to determine the pK(a) values of the amino groups in neomycin B, paromomycin I, and lividomycin A sulfate, with the resulting pK(a) values ranging from 6.92 to 9.51. For each drug, the 3-amino group was associated with the lowest pK(a), with this value being 6.92 in neomycin B, 7.07 in paromomycin I, and 7.24 in lividomycin A. In addition, we use buffer-dependent isothermal titration calorimetry (ITC) to determine the number of protons linked to the complexation of the three drugs with the A site model RNA oligomer at pH 5.5, 8.8, or 9.0. At pH 5.5, the binding of the three drugs to the host RNA is independent of drug protonation effects. By contrast, at pH 9.0, the RNA binding of paromomycin I and neomycin B is coupled to the uptake of 3.25 and 3.80 protons, respectively, with the RNA binding of lividomycin A at pH 8.8 being coupled to the uptake of 3.25 protons. A comparison of these values with the protonation states of the drugs predicted by our NMR-derived pK(a) values allows us to identify the specific drug amino groups whose protonation is linked to complexation with the host RNA. These determinations reveal that the binding of lividomycin A to the host RNA is coupled to the protonation of all five of its amino groups, with the RNA binding of paromomycin I and neomycin B being linked to the protonation of four and at least five amino groups, respectively. For paromomycin I, the protonation reactions involve the 1-, 3-, 2'-, and 2"'-amino groups, while, for neomycin B, the binding-linked protonation reactions involve at least the 1-, 3-, 2', 6'-, and 2"'-amino groups. Our results clearly identify drug protonation reactions as important thermodynamic participants in the specific binding of 2-DOS aminoglycosides to the A site of 16S rRNA.

Anti-Bacterial Agents↗

Exchange behavior of the H-bonded amide protons in the 3 to 13 helix of ribonuclease S.

The preceding article shows that there are eight highly protected amide protons in the S-peptide moiety of RNAase S at pH 5, 0 degrees C. The residues with protected NH protons are 7 to 13, whose amide protons are H-bonded in the 3 to 13 alpha-helix, and Asp 14, whose NH proton is H-bonded to the CO group of Val47. We describe here the exchange behavior of these eight protected protons as a function of pH. Exchange rates of the individual NH protons are measured by 1H nuclear magnetic resonance in D2O. A procedure is used for specifically labeling with 1H only these eight NH protons. The resonance assignments of the eight protons are made chiefly by partial exchange, through correlating the resonance intensities in spectra taken when the peptide is bound and when it is dissociated from S-protein in 3.5 M-urea-d4, in D2O, pH 2.3, -4 degrees C. The two remaining assignments are made and some other assignments are checked by measurements of the nuclear Overhauser effect between adjacent NH protons of the alpha-helix. There is a transition in exchange behavior between pH 3, where the helix is weakly protected against exchange, and pH 5 where the helix is much more stable. At pH 3.1, 20 degrees C, exchange rates are uniform within the helix within a factor of two, after correction for different intrinsic exchange rates. The degree of protection within the helix is only 10 to 20-fold at this pH. At pH 5.1, 20 degrees C, the helix is more stable by two orders of magnitude and exchange occurs preferentially from the N-terminal end. At both pH values the NH proton of Asp 14, which is just outside the helix, is less protected by an order of magnitude than the adjacent NH protons inside the helix. Opening of the helix can be observed below pH 3.7 by changes in chemical shifts of the NH protons in the helix. At pH 2.4 the changes are 25% of those expected for complete opening. Helix opening is a fast reaction on the n.m.r. time scale (tau much less than 1 ms) unlike the generalized unfolding of RNAase S which is a slow reaction. Dissociation of S-peptide from S-protein in native RNAase S at pH 3.0 also is a slow reaction. Opening of the helix below pH 3.7 is a two-state reaction, as judged by comparing chemical shifts with exchange rates. The exchange rates at pH 3.1 are predicted correctly from the changes in chemical shift by assuming that helix opening is a two-state reaction. At pH values above 3.7, the nature of the helix opening reaction changes. These results indicate that at least one partially unfolded state of RNAase S is populated in the low pH unfolding transition.

Amides↗

Cooperative coupling and role of heme a in the proton pump of heme-copper oxidases.

In the last few years, evidence has accumulated supporting the applicability of the cooperative model of proton pumps in cytochrome systems, vectorial Bohr mechanisms, to heme-copper oxidases. The vectorial Bohr mechanism is based on short- and long-range protonmotive cooperative effects linked to redox transitions of the metal centers. The crystal structure of oxidized and reduced bovine-heart cytochrome c oxidase reveals, upon reduction, the occurrence of long-range conformational changes in subunit I of the oxidase. Analysis of the crystal structure of cytochrome c oxidase shows the existence of hydrogen-bonded networks of amino acid residues which could undergo redox-linked pK shifts resulting in transmembrane proton translocation. Our group has identified four proteolytic groups undergoing reversible redox-linked pK shifts. Two groups result in being linked to redox transitions of heme a3. One group is apparently linked to CuB. The fourth group is linked to oxido-reduction of heme a. We have shown that the proton transfer resulting from the redox Bohr effects linked to heme a and CuB in the bovine oxidase displays membrane vectorial asymmetry, i.e., protons are taken up from the inner aqueous space (N), upon reduction, and released in the external space (P), upon oxidation of the metals. This direction of proton uptake and release is just what is expected from the vectorial Bohr mechanism. The group linked to heme a, which can transfer up to 0.9 H+/e- at pHs around neutrality, can provide the major contribution to the proton pump. It is proposed that translocation of pumped protons, linked to electron flow through heme a, utilizes a channel (channel D) which extends from a conserved aspartate at the N entrance to a conserved glutamate located between heme a and the binuclear center. The carboxylic group of this glutamic acid, after having delivered, upon electron flow through heme a, pumped protons towards the P phase, once reprotonated from the N phase, moves to deliver, subsequently, to the binuclear center chemical protons consumed in the conversion of the peroxy to ferryl and of the latter to the oxy intermediate in the redox cycle. Site-directed mutagenesis of protolytic residues in subunit I of the aa3-600 quinol oxidase of Bacillus subtilis to non-polar residues revealed that the conserved Lys 304 is critical for the proton pumping activity of the oxidase. Crystal structures of cytochrome c oxidase show that this lysine is at the N entrance of a channel which translocates the protons consumed for the production of the peroxy intermediate. Inhibition of this pathway, by replacement of the lysine, short-circuits protons from channel D to the binuclear center, where they are utilized in the chemistry of oxygen reduction.

Animals↗

The two pKa's of aspartate-85 and control of thermal isomerization and proton release in the arginine-82 to lysine mutant of bacteriorhodopsin.

To explore the role of Arg82 in the catalysis of proton transfer in bacteriorhodopsin, we replaced Arg82 with Lys, which is also positively charged at neutral pH but has an intrinsic pKa of about 1.7 pH units lower than that of Arg. In the R82K mutant expressed in Halobacterium salinarium, we found the following: (1) The pKa of the purple-to-blue transition at low pH (which reflects the pKa of Asp85) is 3.6 +/- 0.1. At high pH a second inflection in the blue-to-purple transition with pKa = 8.0 is found. The complex titration behavior of Asp85 indicates that the pKa of Asp85 depends on the protonation state of another amino acid residue, X', which has a pKa = 8.0 in R82K. The fit of the experimental data to a model of two interacting residues shows that deprotonation of X' at high pH causes a shift in the pKa of Asp85 from 3.7 to 6.0. In turn, protonation of Asp85 decreases the pKa of X' by 2.3 pH units. This suggests that X' can release a proton upon formation of the M intermediate and the concomitant protonation of Asp85 in the photocycle. (2) The rate constant of dark adaptation, kda, is proportional to the fraction of blue membrane between pH 2 and 10, indicating that thermal isomerization proceeds through the transient protonation of Asp85. The pH dependence of kda shows that two groups with pKal = 3.9 and pKa2 = 8.0 control the rate of dark adaptation in R82K. The 1.7 pH unit shift in pKa2 in R82K compared to the wild type (WT) (pKa2 = 9.7) supports the hypothesis that X' is Arg82 in WT and Lys82 in R82K (or at least that these groups are the principal part of a cluster of residues that constitute X'). (3) Under steady state illumination, the efficiency of proton transport in R82K incorporated in phosphatidylcholine vesicles is at least 40% of that in the WT. A flash-induced transient signal of the pH-sensitive dye pyranine is similar to that in the WT (proton release precedes uptake), but the amplitude is small in R82K (about 15% of that found in the WT), indicating that only a small fraction of protons is released fast in R82K. This supports the suggestions that Arg82 is associated with the proton release pathway (acts as a proton release group or part of a proton release complex) and that Lys cannot efficiently substitute for Arg in this process.(ABSTRACT TRUNCATED AT 400 WORDS)

Arginine↗

The retinal Schiff base-counterion complex of bacteriorhodopsin: changed geometry during the photocycle is a cause of proton transfer to aspartate 85.

Bacteriorhodopsin contains all-trans-retinal linked via a protonated Schiff base to K216. The proton transport in this pump is initiated by all-trans to 13-cis photoisomerization of the retinal and the ensuing transfer of the Schiff base proton to D85. Changed geometrical relationship of the Schiff base and D85 after the photoisomerization is a possible reason for the proton transfer. We introduced small volume/shape changes with site-specific mutagenesis of residues V49 and A53 that contact the side chain of K216, in order to force the Schiff base into somewhat different positions relative to D85. Earlier [Zimányi, L., Váró, G., Chang, M., Ni, B., Needleman, R., & Lanyi, J. K. (1992) Biochemistry 31, 8535-8543] we had described the kinetics of absorbance changes in the microsecond to millisecond time range after photoexcitation with the scheme L<-->M1<-->M2 + H+ (where the first equilibrium is the internal proton transfer and the second is proton release on the extracellular surface). Testing it at various pH values with mutants, where selected rate constants are changed, now confirms the validity of this scheme. The kinetics of the M state thus allowed examination of the transient equilibrium that develops in the L<-->M1 reaction and represents the redistribution of the proton between the Schiff base and D85. From the structure of the protein, the V49A and V49M residue replacements were both predicted to cause decreased alignment of the Schiff base and D85, and indeed we found that they both changed the equilibrium toward the protonated Schiff base. In contrast, the residue replacements A53V and A53G were predicted to move the Schiff base in opposite directions, away from and closer to alignment with D85, respectively. The former indeed changed the equilibrium toward the protonated Schiff base and the latter toward the deprotonated Schiff base. In addition, the hydroxyl stretch band of a bound water in the L state was affected by all mutations that disfavor proton transfer to D85. We conclude that the geometry of the proton donor and acceptor in the Schiff base-D85 pair, mediated by bound water, is a determinant of the proton transfer equilibrium.

Aspartic Acid↗

Retardation of proton transfer caused by binding of the transition metal ion to the bacterial reaction center is due to pKa shifts of key protonatable residues.

Transition metal ions bind to the reaction center (RC) protein of the photosynthetic bacterium Rhodobacter sphaeroides and slow the light-induced electron and proton transfer to the secondary quinone, Q(B). We studied the properties of the metal ion-RC complex by measuring the pH dependence of the dissociation constant and the stoichiometry of proton release upon ligand formation. We investigated the mechanism of inhibition by measuring the stoichiometry and kinetics of flash-induced proton binding, the transfer of (first and second) electrons to Q(B), and the rate of steady-state turnover of the RC in the absence and presence of Cd(2+) and Ni(2+) on a wide pH range. The following results were obtained. (1) The complexation of transition metal ions Cd(2+) and Ni(2+) with the bacterial RC showed strong pH dependence. This observation was explained by different (pH-dependent) states of the metal-ligand cluster: the complex formation was strong when the ligand (Asp and His residues) was deprotonated and was much weaker if the ligand was partly (or fully) protonated. A direct consequence of the model was the pH-dependent proton release upon complexation. (2) The retardation of transfer of electrons and protons to Q(B) was also strongly pH-dependent. The effect was large in the neutral pH range and decreased toward the acidic and alkaline pH values. (3) Steady-state turnover measurements indicated that the rate of the second proton transfer was much less inhibited than that of the first one, which became the rate-limiting step in continuous turnover of the RC. (4) Sodium azide partly recovered the proton transfer rate. The effect is not due to removal of the bound metal ion by azide but probably by formation of a proton-transporting azide network similarly as water molecules may build up proton pathways. (5) We argue that the inhibition comes mainly from pK(a) shifts of key protonatable residues that control the proton transfer along the H-bond network to Q(B). The electrostatic interaction between the metal ion and these residues may result in acidic pK(a) shifts between 1.5 and 2.0 that account for the observed retardation of the electron and proton transfer.

Azides↗

Proton electron-nuclear double-resonance spectra of molybdenum(V) in different reduced forms of xanthine oxidase.

Electron-nuclear double-resonance (ENDOR) spectra of protons coupled to molybdenum(V) in reduced xanthine oxidase samples have been recorded. Under appropriate conditions these protons may be studied without interference from protons coupled to reduced iron-sulfur centers. Spectra have been obtained for the molybdenum(V) species known as Rapid, Slow, Inhibited, and Desulfo Inhibited. Resonances corresponding to at least nine protons or sets of protons are observed for all four species, with coupling constants in the range 0.08-4 MHz. Most of these protons do not exchange when 2H2O is used as solvent. Additional protons giving couplings up to 40 MHz are also detected. These correspond to EPR-detectable protons studied in earlier work. The strongly coupled protons may be replaced by 2H, through appropriate use of 2H2O or of 2H-substituted substrates, with consequent disappearance of the 1H resonances. In most cases the corresponding 2H ENDOR features have also been observed. The nature of the various coupled protons is briefly discussed. Results permit specific conclusions to be drawn about the structures of the Inhibited and Desulfo Inhibited species. In particular, the data indicate that the aldehyde residue of the Inhibited species has been oxidized and that the four protons derived from the ethylene glycol molecule in the Desulfo Inhibited species are not all equivalent. Recent assignments [Edmondson, D.E., & D'Ardenne, S.C. (1989) Biochemistry 28, 5924-5930] of the weakly coupled protons in the latter species appear not to be soundly based. The possibility of obtaining more detailed structural information from the spectra is briefly considered.(ABSTRACT TRUNCATED AT 250 WORDS)

Electron Spin Resonance Spectroscopy↗